a study of cooling system of a spark ignition engine to improve thermal efficiency

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  • 7/30/2019 A Study of Cooling System of a Spark Ignition Engine to Improve Thermal Efficiency

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    A Study of Cooling System of a Spark Ignition Engine to Improve Thermal Efficiency

    Tatsuya Kuboyama1, Yasuo Moriyoshi

    1, Mitsuru Iwasaki

    2and Junichiro Hara

    2

    1Department of Artificial Systems Science, Chiba University, Chiba, Japan

    (Tel : +81-43-290-3916; E-mail: [email protected])2Calsonic Kansei

    Abstract: To improve thermal efficiency of gasoline engines, the effect of coolant system on fuel consumption rate is

    studied in this report. The authors tried to control the flow of cooling water to find an optimized flow system to improve

    thermal efficiency, especially for the cold start condition. Experiments were carried out using a four-cylinder SI engine.

    Three test conditions of i) normal cold start, ii) cold start without operating the water pump and iii) cold start but with

    heated engine oil were measured. Temperatures of cooling water at some positions were measured during the

    warming-up time. Secondly, the effect of cooling water temperature on thermal efficiency at a steady state condition wasexamined. As a result, a higher temperature causes an improvement of thermal efficiency due to a reduction i n

    mechanical friction.

    Keywords: Gasoline engine, Thermal efficiency, Cooling system, Cooling water temperature

    1. INTRODUCTION

    Improvement of thermal efficiency has been strongly

    demanded for internal combustion engines. One of themethods to increase theoretical thermal efficiency is an

    increase in compression ratio. However, the increase

    in compression ratio is limited by knocking. A

    reduction in energy loss including cooling loss and

    mechanical friction also improves brake thermal

    efficiency. It is well known that cooling watertemperature and combustion chamber wall temperature

    largely affect cooling loss and knocking. Temperatureof lubricant oil affects mechanical friction. High oil

    temperature reduces oil viscosity leading to decreasing

    friction loss. In summary, thermal management has

    been more important for combustion engines forimproving thermal efficiency. In recent days,

    electrically controlled water pump and electric thermo-

    stat have been utilized to optimize cooling water

    temperature according to operating conditions[1], [2].

    It is considered that the development of these

    electrically controllable devices allows more precise

    thermal management for improvement in performance

    of gasoline engines.

    In the present study, as a first step to develop asophisticated controlling method for a cooling system of

    a gasoline engine, thermal efficiency during cold

    start operation and steady state operation were

    experimentally investigated using a

    commercially available four-cylinder gasoline

    engine.

    2. TEST ENGINE AND CONDITIONS

    Table 1 shows the specifications of the test engine. Acommercially available four-cylinder gasoline engine

    was used. The engine has a displacement volume of

    1240 cm3, and a compression ratio of 9.8. The ECU

    (Electronic control unit) which is normally applied to

    production engine was used for controlling of engine

    operating parameters, such as an ignition timing and a

    fuel injection timing. Figure 1(a) shows cooling water

    path and measurement locations of cooling watertemperature for cold start testing. During the warm up

    period, thermo-stat closes, and cooling water circulates

    through the bypass. After a cooling water temperature

    increases, thermo-stat opens, and cooling water

    circulates through the radiator which is soaked in the

    water tank. Figure 1(b) shows a cooling water pathand measurement locations of wall temperature for

    steady state testing. In the steady state testing, thecoolant water path for the cylinder block and that for the

    cylinder head are separated. This allows independent

    control of temperature and flow rate of cooling water

    for the cylinder head and the cylinder block of the testengine.

    In this system, temperature in the water tank is

    controlled. A cooling water temperature is not directly

    controlled but determined by the water tank temperature

    and operating conditions. Cooling water temperature

    was measured at ten locations shown in figure 1 (Ch 1

    Ch 10) during cold start experiment. Additionally,

    intake and exhaust gas temperature, cylinder head wall

    temperature at the spark plug location was measured.In-cylinder pressure of #3 cylinder was measured by a

    piezo-electric pressure transducer (Kister 6117B).

    Concentrations of exhaust emissions including CO, O2,

    NO, HC, CO2 and mass ratio of air to fuel (A/F) were

    measured by an exhaust gas analyzer (HORIBA,

    MEXA-584L).

    Experiments were carried out during cold start

    condition and steady state conditions. During the cold

    star testing, the engine operation was started with a

    cooling water temperature of 25oC, and the cooling

    water temperature and exhaust emissions were

    measured for 15 minutes with a sampling rate of 1 Hz.

    In-cylinder pressure of #3 cylinder was measured at twotimes, at 4 minutes and 13 minutes after start of engine

    SICE Annual Conference 2011September 13-18, 2011, Waseda University, Tokyo, Japan

    PR0001/11/0000-0467 400 2011 SICE- 467 -

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    operation.

    The cold start testing was conducted with threedifferent conditions.

    a) Normal cold start operationb) Cold start operation without operating a water

    pump. In this case, cooling water did not circulate

    during warm up duration.c) Initial temperature of lubricant oil increases up to

    100oC.

    Table1 Engine specifications

    Engine TypeIn-line

    4-cylinder

    Compression ratio 9.8

    Displacement [cc] 310.0

    Bore x Stroke [mm] 71.0 x 78.3

    Connecting rod length [mm] 120.75

    Idle speed [r/min] 700

    Thermostat open temperature [oC] 821.5

    Thermostat close temperature [oC] 77

    In the steady state testing, to investigate the effect of

    cooling water temperature on thermal efficiency,

    cooling water temperature for the cylinder block and

    that for the cylinder head were varied as shown in Table

    2. Mass averaged cooling water temperature was fixed

    among the three cases. A higher cooling water

    temperature for cylinder head would have effect on

    indicated thermal efficiency because the cylinder head

    wall temperature affects combustion characteristics and

    knocking limit. Also, a higher cooling water

    temperature for the cylinder block is expected toimprove a brake thermal efficiency by reducing

    mechanical friction due to an increase in lubricant oil

    temperature. In this experiment, the engine was

    running at 2000 rpm. Spark timing was set at the

    minimum advance for best torque (MBT). The engine

    load was varied from IMEP of 300 kPa to 900 kPa.

    Table 2. Experimental conditions

    Cylinder block

    coolant water

    temp. C

    Cylinder head

    coolant water

    temp. C

    Case 1 80 C 80 C

    Case 2 60 C 100 C

    Case 3 100 C 60 C

    3. RESULTS AND DISCUSSION

    3.1 Effect of cooling system on engine performance

    during cold start condition

    Figure 2 shows temporal variation in cooling water

    temperature during cold start testing.With a normal cold start operation (a), cooling water

    temperature increases during warming up operation

    (until 590 sec after start of engine operation). This isbecause the thermo-stat does not work during warming

    Fig.1(a) Cooling water path and cooling watertemperature measurement locations for cold start

    experiment

    Figure 1 (b) Cooling water path and wall

    temperature measurement locations for steady stateexperiment

    up operation. It is found that difference in measured

    temperature at location Ch 2 and Ch 8 is 20oC. This

    indicates that there is temperature difference between

    the cylinders. Cylinder wall temperature distribution

    should be reduced to improve total performance of agasoline engine, because engine operating parameters,

    such as ignition timing, are determined and restricted by

    the worst cylinder. Once a cooling water temperature

    increases (after 590 sec. from start of engine operation),temperature of cooling water suddenly decreases. This

    is because the thermo-stat begins to work, and relatively

    low temperature cooling water is introduced into the

    engine cooling path from the radiator. Shortly after the

    decrease in cooling water temperature, the thermo-stat

    closes again, and cooling water temperature increases.After warming up operation, cooling water temperature

    is kept constant.

    In case that the water pump is stopped during warmup operation (b), cooling water temperature increases

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    even though thermo-stat opens because low temperature

    water is not introduced.In case that the initial lubricant oil temperature

    increases up to 100oC, temporal variation in cooling

    water temperature is similar to the normal cold start

    conditions. However, warm up duration decreases by

    approximately 95 seconds. High temperature oilwould warm up engine components. This would reducewarm up duration. The similar variation in cooling

    water temperature between different measurement

    locations to the normal cold start operation is observed

    in the case (b) and (c). It could be concluded that the

    cooling water temperature distribution during cold start

    operation would not be affected by cooling watercirculation and lubricant oil temperature. To realize

    uniform water temperature distribution and uniform

    cylinder wall temperature distribution, a basic design of

    the cooling water path must be optimized.

    0

    20

    40

    60

    80

    100

    120

    140

    0 300 600 900

    Time[sec]

    Temperature[]

    CH1

    CH2

    CH7

    CH8

    (a) normal cold start condition

    0

    20

    40

    60

    80

    100

    120

    140

    0 300 600 900

    Time[sec]

    Temperature[

    ]

    CH1

    CH2

    CH7

    CH8

    (b) cold start w/o water pump condition

    0

    20

    40

    60

    80

    100

    120

    140

    0 300 600 900

    Time[sec]

    Temperature[]

    CH1

    CH2

    CH7CH8

    (c) cold start with initially warmed oil

    condition

    Fig.2 Temporal variations of coolant temp.

    Figure 3 shows engine speed, exhaust gas

    temperature, lubricant oil temperature during cold start

    operation. It can be seen that the difference in the

    experimental conditions does not affects engine speed

    and exhaust gas temperature. Figure 4 shows fuelconsumption rate and cumulative fuel consumption. The

    engine operation started 2 seconds after start of data

    acquisition. From these figures, it can be seen that a

    large amount of fuel is consumed during first 5 seconds

    after start of engine operation. It is also found that the

    amount of fuel consumed during cold start with normal

    operation (a) is largest among the three cases. Fuel

    consumption with high initial oil temperature is lowest.

    Fuel consumption during cold start operation could beimproved by 2.6 % with stopping cooling water

    circulation, and by 3.5 % with an initial high

    temperature lubricant oil.

    (a) Engine speed

    (b) Exhaust gas temperature

    (c) Lubricant oil temperatureFig.3 Temporal variation engine speed, exhaust

    gas temperature and lubricant oil temperature

    for different cold start conditions

    3.2 Effect of cooling system on engine performance

    during steady state operation

    Figure 5 shows effect of cooling water temperature

    on cylinder head wall temperature. It is found that

    cylinder head temperature increases with increasingcoolant water temperature on cylinder head. Also, it

    0

    200

    400

    600

    800

    1000

    1200

    1400

    1600

    1800

    0 300 600 900

    Time[sec]

    Enginespeed[r/min]

    Normal

    Without belt

    Hot oil start

    0

    50

    100

    150

    200

    250

    300

    350

    400

    0 300 600 900

    Time[sec]

    Temperature[]

    Normal

    Without belt

    Hot oil start

    0

    10

    20

    30

    40

    50

    60

    70

    0 300 600 900

    Time[sec]

    Temperature[]

    Normal

    Without belt

    Hot oil start

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    can be seen that the exhaust side wall temperature is

    more sensitive to the cooling water temperature.Figure 6 shows effect of cooling water temperature on

    thermal efficiency. Indicated thermal efficiency was

    not affected by the cooling water temperature.

    However, brake thermal efficiency could be improved

    by increasing the cooling water temperature for thecylinder block. Brake thermal efficiency with Case 3(Block 100

    oC) was improved by 3 to 5%, compared to

    Case 1(Block 80oC). This is probably because of a

    reduction in mechanical friction due to an increase in

    lubricant oil temperature with the increase in a cooling

    water temperature for the cylinder block. From the

    results obtained in this study suggest that thermalefficiency could be improved by appropriate controlling

    of cooling water temperature depending on the

    operational conditions. As a next step, the authors will

    try to develop a controlling strategy of cooling water

    temperature for improving a thermal efficiency.

    (a) Fuel mass flow rate

    (b) Fuel mass flow rate (expanded)

    (c) Cumulative fuel consumption during coldstart oeration

    Fig.4 Effect of cold start conditions on fuelconsumption

    Fig. 5 The effect of coolant water temperature oncylinder head wall temperature

    (upper: intake side, lower: exhaust side)

    Fig.6. The effect of coolant water temperature on

    thermal efficiency and mechanical loss

    0

    0.5

    1

    1.5

    2

    2.5

    0 300 600 900

    Time[sec]

    Gasolinemassflow

    rate[g/s]

    Normal

    Without belt

    Hot oil start

    0

    0.5

    1

    1.5

    2

    2.5

    0 5 10 15 20

    Time[sec]

    Gasolinemassflow

    rate[g/s]

    Normal

    Without belt

    Hot oil start

    0

    2

    4

    6

    8

    10

    12

    0 5 10 15 20

    Time[sec]

    Gasolinemassflow

    rate[g]

    Normal

    Without belt

    Hot oil start

    80

    90

    100

    110

    120

    130

    140

    150

    160

    #1 #2 #3 #4

    Walltemp.

    (Intakeside)oC

    Cylinder number

    Head 80/Block 80

    Head 100/Block 60

    Head 60/Block 100

    80

    90

    100

    110

    120

    130

    140

    150

    160

    #1 #2 #3 #4

    Walltempe.(Exh.side)oC

    Cylinder number

    Head 80/Block 80Head 100/Block 60

    Head 60/Block 100

    15

    20

    25

    30

    35

    40

    0 200 400 600 800 1000Brakethermalefficiency%

    IMEP kPa

    Head 60/Block 100

    Head 80/Block 80

    Head 100/Block 60

    15

    20

    25

    30

    35

    40

    0 200 400 600 800 1000

    Brakethermalefficiency%

    IMEP kPa

    Head 60/Block 100

    Head 80/Block 80

    Head 100/Block 60

    10

    15

    20

    25

    30

    35

    40

    0 200 400 600 800 1000

    Mechanicalloss%

    IMEP kPa

    Head 60/Block 100

    Head 80/Block 80

    Head 100/Block 60

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    4. SUMMARY

    As a first step of developing a control strategy of

    cooling system of gasoline engines for improvement in

    thermal efficiency, thermal efficiency during cold start

    operation and steady state operation were

    experimentally investigated using a commerciallyavailable four-cylinder gasoline engine. Experimental

    results can be summarized as follows;

    (1) Fuel consumption during cold start operation couldbe improved by 2.6 % with stopping cooling water

    circulation, and by 3.5 % with an initial high

    temperature lubricant oil.

    (2) During cold start operation, a spatial distribution ofcooling water temperature which would result in

    wall temperature variation between the cylinder

    was not affected by oil temperature and cooling

    water circulation. This indicates that a basicdesign of the cooling water path is dominant factor

    for the spatial distribution of a cooling water

    temperature.

    (3) A higher cooling water temperature for the cylinderblock could improve brake thermal efficiencyduring steady state operation because of a reduction

    in mechanical friction. With the increase in

    cooling water temperature for the cylinder block

    from 60oC to 100

    oC, break thermal efficiency was

    improved by 3 to 5%.

    ACKNOWLEDGEMENT

    The authors would like to thankKistler Japan, Co.

    ltd., for their support in the pressure

    measurements. Mr. S, Notoya and K. Toida of

    Chiba University are also acknowledged for theirsupport in the experimental works.

    REFERENCES

    [1] E.Sonntag et al., The New Family of Small 4

    -Cylinder Engines, JSAE paper No.20075365, 2007.[2] A. Eiser et al., The new 1.8L TFSI engine from

    Audi, Part 1 Base engine and Thermo-management,

    MTZ vol. 72, pp. 23- 39, 2011.

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